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Course Information for Math 311 by Dr. Craig Johnson |
Trajectories in the phase plane of a
2x2 first-order system. The eigenvalues are real and of
opposite sign. The study of ordinary differential
equations and first-order systems (linear and nonlinear)
through a combination of analytical, numerical, and
qualitative techniques. Topics include direction fields,
solving first order equations of several types, solving
second order linear equations, the Laplace transform, first
order systems, phase plane portraits, and classification of
equilibrium points. The textbook is "Elementary
Differential Equations" by Boyce/DiPrima and published by
Wiley. The course grade is determined by 3 tests, 4 homework
sets, 2 Maple computer labs, a semester project, and the
final examination. The project must
demonstrate a substantial application of differential
equations. Related articles from the
American Mathematical Monthly and
useful websites for the course are listed
at the end of this page. Prerequisite: Calculus
II

Section Topic Section Topic Section Topic 1.1 Direction Fields 3.1 Homogeneous Eqns 6.1 Laplace Transform 1.2 Some solutions of DE's 3.2 Fundamental Solns 6.2 Solution of IVP's 1.3 Classification of ODE's 3.3 Linear Independence 6.6 Convolution Integral 2.1 Linear Equations 3.4 Complex Roots 7.2 Review of Matrices 2.2 Separable Equations 3.5 Repeated Roots 7.3 Eigenvectors 2.3 Modeling 3.6 Undetermined Coeffts 7.4 Systems of 1st order de 2.4 Differences of Lin vs Nonlin 3.7 Variation of Parameters 7.5 Homog. Linear Systems 2.5 Autonomous Eqns 3.8 Mech & Electrical Vibrations 7.6 Complex Eigenvalues 2.6 Exact Eqns 4.1 Theory of nth order eqns 7.8 Repeated Eigenvalues 2.7 Euler's Method 4.2 Homog. nth order eqns 9.1 The Phase Plane 2.8 Existence and Uniqueness 9.2 Autonomous Systems
Sample Abstracts of Projects from Fall, 2000
Past Project Titles
Modeling physical, biological, and social phenomena using differential equations is a powerful tool for providing attainable answers to obscure questions. In this case, a non-linear system of first-order equations is used to model the way a disease spreads through a population.
dy/dt = a x(t) y(t) - b y(t)
Here x(t) represents the number of people who are susceptible to the disease and y(t) represents the number of people who are currently infected with the disease. The group of susceptibles is reduced by one person each time one of them becomes infected. One relevant question is, "When does infection occur?" Infection can occur during the times when susceptibles are in contact with infecteds. Therefore, the rate of change dx/dt of the number of susceptibles is proportional to the product of x(t) and y(t). The first equation above reflects this where a > 0 is a constant that measures how fast the disease is transmitted. The second equation is derived from the fact that the rate of change dy/dt of infecteds is likewise positively affected by the product of x(t) and y(t) but negatively affected by the current population y(t). In other words, the rate slows as y(t) increases.
This system was solved numerically by Maple 6 using feasible values for a and b and initial conditions provided by examining AIDS data for the state of Pennsylvania from 1990 to the present. The vector field and trajectory are shown below.

The graphs for x and y versus t were then compared to the actual data. A reasonable match was then found by modifying the values of a and b.
The rate of a chemical reaction is the change in concentration of a substance per unit time. During a reaction the concentration of reactants decrease and the products increase. Different expermental techniques are used to guage the rate of a reaction such as colour, pH, and electric conductivity. Readings are taken at definite time intervals which allows the prediction of the rate at any concentration. The relation between the rate and the concentration can be mathematically set up as a system of first-order differential equations. For a simple reaction x + y --> z, the representation could be:
dy/dt = -k2 (x^m)(y^n)
where x(t), y(t) are the amounts of the involved substances at time t. The parameters m and n are the orders of the reaction with respect to x and y respectively. Such systems are useful because they allow us to predict how a reaction will proceed and, in particular, can assist in controlling the reactions in organic chemistry where every step and rate must be precisely controlled in order to get desired products. I used Maple 6 to find numerical solutions to this system for various initial conditions and reaction orders. It is interesting to determine when the substances achieve equilibrium depending on whether x(0) > y(0) or x(0) < y(0).
The behavior of a physical system like the weather on Earth is extremely complicated and so long-range forecasts have had limited success.In 1963 Edward Lorenz was a meterologist who devised a simplified three-dimensional system of first-order equations to mathematically model the weather in order to make predictions.
dy/dt = rx - y - xz
dz/dt = -bz + xy
This simple system led to the field of Chaos Theory. Chaos deals with the largely unpredictable evolution occurring in a deterministic, nonlinear, dynamical system because of sensitivity to initial conditions. This paper finds the equilibrium points to the system for specific values of the parameters s, r, and b. It also uses the Euler method to find numerical solutions for several sets of slightly different initial conditions. Graphs of the x, y, and z functions are given to demonstrate the unpredictablility of the long-term behavior.
Human learning, or more specifically the rate of memorization, is a complicated process. This paper explores the model presented in Differential Equations by Blanchard, Devaney, and Hall on p. 133. It is based on the assumption that the rate of learning is proportional to the amount left to be learned. We let L(t) be the fraction of a list of numbers already committed to memory at time t. So L = 0 corresponds to knowing none of the list and L = 1 corresponds to knowing the entire list. The differential equation is
The parameter k depends on a particular individual's rate of learning. It can be determined through experimentation and so I chose to study my personal rate of memorization to determine my k-value. I began by studying a random list of 20 numbers, each consisting of 3 digits, for one minute. I then attempted to recreate as much of the list as possible from my memory in the correct order. I then spent another minute studying the same list of numbers and quizzed myself again. This process continued until I learned the entire list. It wasn't until after learning the entire list that I went back and graded my "quizzes". I then repeated the process for two more lists. I then applied exponential regression techniques to graphs of L versus t to find a function for L(t) and compared it to the solution for the above differential equation. Finally, I modified the above equation to
and compared the regression fits to the solution to this equation. These seemed to be a better match. I think much more analysis could be done to also account for other factors that affect the learning process.
http://www.mapleapps.com/index.asp (The Maple Applications Center)
http://math.bu.edu/odes (Boston University D.E. projects)
http://diffeq.brookscole.com (Brooks/Cole D.E. Resource Site)
http://www.maa.org (Mathematical Association of America)
http://math.duke.edu/education/ccp/materials/diffcalc/sir/sir3.html(D.E. model for the spread of disease)
Useful Articles from the American Mathematical Monthly
Marywood University <|> Undergraduate School <|> Undergraduate Admissions
Comments to Dr. Craig M. Johnson, Chair, Dept. of Mathematics: johnsonc@ac.marywood.edu
Last update: January 29, 2001
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